GB1069754A - Improvements in apparatus for x-ray analysis of a material - Google Patents

Improvements in apparatus for x-ray analysis of a material

Info

Publication number
GB1069754A
GB1069754A GB23010/64A GB2301064A GB1069754A GB 1069754 A GB1069754 A GB 1069754A GB 23010/64 A GB23010/64 A GB 23010/64A GB 2301064 A GB2301064 A GB 2301064A GB 1069754 A GB1069754 A GB 1069754A
Authority
GB
United Kingdom
Prior art keywords
filter
specimen
wavelength
radiation
determination
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired
Application number
GB23010/64A
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Individual
Original Assignee
Individual
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Individual filed Critical Individual
Publication of GB1069754A publication Critical patent/GB1069754A/en
Expired legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N23/00Investigating or analysing materials by the use of wave or particle radiation, e.g. X-rays or neutrons, not covered by groups G01N3/00 – G01N17/00, G01N21/00 or G01N22/00
    • G01N23/22Investigating or analysing materials by the use of wave or particle radiation, e.g. X-rays or neutrons, not covered by groups G01N3/00 – G01N17/00, G01N21/00 or G01N22/00 by measuring secondary emission from the material
    • G01N23/223Investigating or analysing materials by the use of wave or particle radiation, e.g. X-rays or neutrons, not covered by groups G01N3/00 – G01N17/00, G01N21/00 or G01N22/00 by measuring secondary emission from the material by irradiating the sample with X-rays or gamma-rays and by measuring X-ray fluorescence
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N2223/00Investigating materials by wave or particle radiation
    • G01N2223/07Investigating materials by wave or particle radiation secondary emission
    • G01N2223/076X-ray fluorescence

Landscapes

  • Physics & Mathematics (AREA)
  • Health & Medical Sciences (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Chemical & Material Sciences (AREA)
  • Analytical Chemistry (AREA)
  • Biochemistry (AREA)
  • General Health & Medical Sciences (AREA)
  • General Physics & Mathematics (AREA)
  • Immunology (AREA)
  • Pathology (AREA)
  • Analysing Materials By The Use Of Radiation (AREA)

Abstract

1,069,754. Photo-electric X-ray analysis. J. BAECKLUND. June 3, 1964 [June 7, 1963], No. 23010/64. Heading G1A. [Also in Division H5] In apparatus for the analysis of a specimen by X-rays, a filter 2 (Fig. 1) is interposed between the X-ray tube 1 and the specimen 3, the filter having a high absorptivity within a range of wavelengths containing a definite wavelength to be considered, and a low absorptivity at shorter wavelengths. When the specimen is to be analyzed to determine the concentration of a particular constituent element, some of the primary radiation from the X-ray tube anode is scattered from the sample and forms a background specimen on which the characteristic fluorescent radiation of the sample is superimposed. If the particular wavelength of the constituent to be considered coincides with the characteristic lines of the X-ray source, the accuracy of the measurements will be affected. To counteract this, instead of replacing the X-ray tube by one with a different anode material, a filter of an element dependent on the anode material, is interposed as stated above. For example, in the analysis of a steel specimen, for the determination of the chromium content, when a chromium anode is used, the background radiation Fig. 2 (not shown) has a peak at the wavelength which is to be used in the measurement of the chromium content. The interposition of a titanium filter (having an absorption characteristic as in Fig. 3, not shown) reduces the unwanted line to reasonable proportions Fig. 4 (not shown). The shorter wavelength primary radiation which produces the fluorescent radiation of the specimen, is passed by the filter with little attenuation. In the determination of lead, tantalum or bismuth in steel, a tin filter is necessary. The apparatus is designed so that the filter for the determination of a particular constituent can be switched in when needed. This is decided by the angular displacement of the detector 6 with respect to the diffraction crystal 5. A number of filters are therefore carried in a special mount Fig. 7 (not shown) attached to a permanent magnet and coil arrangement, operated by signals from a switching unit controlled by the actuation mechanism which displaces the detector 6.
GB23010/64A 1963-06-07 1964-06-03 Improvements in apparatus for x-ray analysis of a material Expired GB1069754A (en)

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
SE633963 1963-06-07

Publications (1)

Publication Number Publication Date
GB1069754A true GB1069754A (en) 1967-05-24

Family

ID=20268425

Family Applications (1)

Application Number Title Priority Date Filing Date
GB23010/64A Expired GB1069754A (en) 1963-06-07 1964-06-03 Improvements in apparatus for x-ray analysis of a material

Country Status (4)

Country Link
US (1) US3402292A (en)
DE (1) DE1245174B (en)
GB (1) GB1069754A (en)
NL (1) NL6406437A (en)

Families Citing this family (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5111429Y1 (en) * 1969-03-29 1976-03-27
JPS515316B1 (en) * 1969-09-25 1976-02-19
US3801785A (en) * 1972-11-01 1974-04-02 Raytheon Co Spatially modulated imaging system
US3860817A (en) * 1973-08-10 1975-01-14 Gen Electric Reducing patient X-ray dose during fluoroscopy with an image system
US4499591A (en) * 1982-11-17 1985-02-12 Gary Hartwell Fluoroscopic filtering
NL8400845A (en) * 1984-03-16 1985-10-16 Optische Ind De Oude Delft Nv DEVICE FOR GAP RADIOGRAPHY.
US5778041A (en) * 1983-10-13 1998-07-07 Honeywell-Measurex Corporation System and process for measuring ash in paper
DE3500812A1 (en) * 1985-01-11 1986-07-17 Siemens AG, 1000 Berlin und 8000 München X-RAY DIAGNOSTIC DEVICE WITH SEMI-TRANSPARENT PANEL
US4860329A (en) * 1986-02-24 1989-08-22 Upa Technology, Inc. X-ray fluorescence thickness measuring device
US4987582A (en) * 1989-10-19 1991-01-22 Hughes Aircraft Company X-ray fluorescence imaging of elements

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3079499A (en) * 1959-06-19 1963-02-26 Hilger & Watts Ltd X-ray beam intensity responsive sequential spectrometer
US3218458A (en) * 1960-02-29 1965-11-16 Picker X Ray Corp Diffractometer

Also Published As

Publication number Publication date
NL6406437A (en) 1964-12-08
DE1245174B (en) 1967-07-20
US3402292A (en) 1968-09-17

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